Vibrational Frequencies calculated at LSDA/6-31+G**
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A |
3753 |
3697 |
70.37 |
|
|
|
| 2 |
A |
3238 |
3189 |
5.26 |
|
|
|
| 3 |
A |
3089 |
3043 |
15.42 |
|
|
|
| 4 |
A |
1433 |
1411 |
8.68 |
|
|
|
| 5 |
A |
1302 |
1282 |
4.86 |
|
|
|
| 6 |
A |
1238 |
1220 |
122.22 |
|
|
|
| 7 |
A |
1010 |
995 |
55.28 |
|
|
|
| 8 |
A |
496 |
489 |
208.59 |
|
|
|
| 9 |
A |
367 |
361 |
6.22 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7962.8 cm
-1
Scaled (by 0.985) Zero Point Vibrational Energy (zpe) 7843.3 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.316 |
|
|
|
| 2 |
O |
-0.384 |
|
|
|
| 3 |
H |
0.173 |
|
|
|
| 4 |
H |
0.156 |
|
|
|
| 5 |
H |
0.370 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.216 |
1.665 |
0.246 |
1.696 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.967 |
2.368 |
-0.671 |
| y |
2.368 |
-11.217 |
-0.007 |
| z |
-0.671 |
-0.007 |
-15.198 |
|
| Traceless |
| | x | y | z |
| x |
1.241 |
2.368 |
-0.671 |
| y |
2.368 |
2.365 |
-0.007 |
| z |
-0.671 |
-0.007 |
-3.606 |
|
| Polar |
| 3z2-r2 | -7.212 |
| x2-y2 | -0.750 |
| xy | 2.368 |
| xz | -0.671 |
| yz | -0.007 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.298 |
0.036 |
0.024 |
| y |
0.036 |
2.490 |
-0.017 |
| z |
0.024 |
-0.017 |
2.728 |
<r2> (average value of r
2) Å
2
| <r2> |
20.858 |
| (<r2>)1/2 |
4.567 |